Robert M. Sweet

Crystal structures of myoglobin-ligand complexes at near-atomic resolution.

We have used x-ray crystallography to determine the structures of sperm whale myoglobin (Mb) in four different ligation states (unligated, ferric aquomet, oxygenated, and carbonmonoxygenated) to a resolution of better than 1.2 A. Data collection and analysis were performed in as much the same way as possible to reduce model bias in differences between structures. The structural differences among the ligation states are much smaller than previously estimated, with differences of <0.25 A root-mean-square deviation among all atoms. One structural parameter previously thought to vary among the ligation states, the proximal histidine (His-93) azimuthal angle, is nearly identical in all the ferrous complexes, although the tilt of the proximal histidine is different in the unligated form. There are significant differences, however, in the heme geometry, in the position of the heme in the pocket, and in the distal histidine (His-64) conformations. In the CO complex the majority conformation of ligand is at an angle of 18 +/- 3 degrees with respect to the heme plane, with a geometry similar to that seen in encumbered model compounds; this angle is significantly smaller than reported previously by crystallographic studies on monoclinic Mb crystals, but still significantly larger than observed by photoselection. The distal histidine in unligated Mb and in the dioxygenated complex is best described as having two conformations. Two similar conformations are observed in MbCO, in addition to another conformation that has been seen previously in low-pH structures where His-64 is doubly protonated. We suggest that these conformations of the distal histidine correspond to the different conformational substates of MbCO and MbO(2) seen in vibrational spectra. Full-matrix refinement provides uncertainty estimates of important structural parameters. Anisotropic refinement yields information about correlated disorder of atoms; we find that the proximal (F) helix and heme move approximately as rigid bodies, but that the distal (E) helix does not.

A 9 Å Resolution X-Ray Crystallographic Map of the Large Ribosomal Subunit

The 50S subunit of the ribosome catalyzes the peptidyl-transferase reaction of protein synthesis. We have generated X-ray crystallographic electron density maps of the large ribosomal subunit from Haloarcula marismortui at various resolutions up to 9 A using data from crystals that diffract to 3 A. Positioning a 20 A resolution EM image of these particles in the crystal lattice produced phases accurate enough to locate the bound heavy atoms in three derivatives using difference Fourier maps, thus demonstrating the correctness of the EM model and its placement in the unit cell. At 20 A resolution, the X-ray map is similar to the EM map; however, at 9 A it reveals long, continuous, but branched features whose shape, diameter, and right-handed twist are consistent with segments of double-helical RNA that crisscross the subunit.

Structure determination and refinement of bovine lens leucine aminopeptidase and its complex with bestatin

The three-dimensional structure of bovine lens leucine aminopeptidase (EC 3.4.11.1) complexed with bestatin, a slow-binding inhibitor, has been solved to 3.0 A resolution by the multiple isomorphous replacement method with phase combination and density modification. In addition, this structure and the structure of the isomorphous native enzyme have been refined at 2.25 and 2.32 A resolution, respectively, with crystallographic R-factors of 0.180 and 0.159, respectively. The current structural model for the enzyme includes the two zinc ions and 481 of the 487 amino acid residues comprising the asymmetric unit. The enzyme is physiologically active as a hexamer, which has 32 symmetry, and is triangular in shape with a triangle edge length of 115 A and maximal thickness of 90 A. Monomers are crystallographically equivalent. Each is folded into two unequal alpha/beta domains connected by an alpha-helix to give a comma-like shape with approximate maximal dimensions of 90 A x 55 A x 55 A. The secondary structural composition is 35% alpha-helix and 23% beta-strand. The N-terminal domain (160 amino acid residues) mediates trimer-trimer interactions and does not appear to participate directly in catalysis, while the C-terminal domain (327 amino acid residues) is responsible for catalysis and binds the two zinc ions, which are less than 3 A apart. These two metal ions are located near the edge of an eight-stranded, saddle-shaped beta-sheet. The zinc ion that has the lower temperature factor is co-ordinated by one carboxylate oxygen atom from each of Asp255, Asp332 and Glu334, and the carbonyl oxygen of Asp332. The other zinc ion, presumed to be readily exchangeable, is co-ordinated by one carboxylate oxygen atom of each of Asp273 and Glu334 and the side-chain amino group of Lys250. The active site also contains two positively charged residues, Lys262 and Arg336. The six active sites are themselves located in the interior of the hexamer, where they line a disk-shaped cavity of radius 15 A and thickness 10 A. Access to this cavity is provided by solvent channels that run along the 2-fold symmetry axes. Bestatin binds to one of the active site zinc ions, and its phenylalanine and leucine side-chains occupy hydrophobic pockets adjacent to the active site. Finally, the relationship between bovine lens leucine aminopeptidase and the homologous enzyme pepA from Escherichia coli is discussed.

The structure of a chromosomal high mobility group protein-DNA complex reveals sequence-neutral mechanisms important for non-sequence-specific DNA recognition.

The high mobility group (HMG) chromosomal proteins, which are common to all eukaryotes, bind DNA in a non‐sequence‐specific fashion to promote chromatin function and gene regulation. They interact directly with nucleosomes and are believed to be modulators of chromatin structure. They are also important in V(D)J recombination and in activating a number of regulators of gene expression, including p53, Hox transcription factors and steroid hormone receptors, by increasing their affinity for DNA. The X‐ray crystal structure, at 2.2 Å resolution, of the HMG domain of the Drosophila melanogaster protein, HMG‐D, bound to DNA provides the first detailed view of a chromosomal HMG domain interacting with linear DNA and reveals the molecular basis of non‐sequence‐specific DNA recognition. Ser10 forms water‐mediated hydrogen bonds to DNA bases, and Val32 with Thr33 partially intercalates the DNA. These two ‘sequence‐neutral’ mechanisms of DNA binding substitute for base‐specific hydrogen bonds made by equivalent residues of the sequence‐specific HMG domain protein, lymphoid enhancer factor‐1. The use of multiple intercalations and water‐mediated DNA contacts may prove to be generally important mechanisms by which chromosomal proteins bind to DNA in the minor groove.

Atomic structure of an alphabeta T cell receptor (TCR) heterodimer in complex with an anti-TCR fab fragment derived from a mitogenic antibody.

Each T cell receptor (TCR) recognizes a peptide antigen bound to a major histocompatibility complex (MHC) molecule via a clonotypic αβ heterodimeric structure (Ti) non‐covalently associated with the monomorphic CD3 signaling components. A crystal structure of an αβ TCR‐anti‐TCR Fab complex shows an Fab fragment derived from the H57 monoclonal antibody (mAb), interacting with the elongated FG loop of the Cβ domain, situated beneath the Vβ domain. This loop, along with the partially exposed ABED β sheet of Cβ, and glycans attached to both Cβ and Cα domains, forms a cavity of sufficient size to accommodate a single non‐glycosylated Ig domain such as the CD3ϵ ectodomain. That this asymmetrically localized site is embedded within the rigid constant domain module has implications for the mechanism of signal transduction in both TCR and pre‐TCR complexes. Furthermore, quaternary structures of TCRs vary significantly even when they bind the same MHC molecule, as manifested by a unique twisting of the V module relative to the C module.

Structure of a Monoclinic Crystal Form of Cytochrome b1 (Bacterioferritin) from E. coli

Crystals of E. coli cytochrome b1, alias bacterioferritin, were grown fr om a low ionic strength solution. The resulting monoclniic P21 structure was solved by molecular replacement and refined using noncrystallographi c symmetries applied to the fundamental unit, consisting of two protein subunits and a single haem. From the Patterson self-rotation results it was shown that the asymmetric unit of the monoclinic crystal consists of 12 such dimers and corresponds to a complete, nearly spherical, molecule of bacterioferritin (M4 = 450 kDa) of 432 point-group symmetry. It is thus the most symmetrical cytochrome. As previously determined for the tetragonal form, the haem is located in a special position on a local twofold axis of the dimer. A bimetal centre is also observed within the four-helix bundle of each monomer; a metal-binding site is located on the fourfold axis.

PROTEIN DATA BANK DEPOSITIONS FROM SYNCHROTRON SOURCES

A survey and analysis of Protein Data Bank (PDB) depositions from international synchrotron radiation facilities, based on the latest released PDB entries, are reported. The results (http://asdp.bnl.gov/asda/Libraries/) show that worldwide, every year since 1999, more than 50% of the deposited X-ray structures have used synchrotron facilities, reaching 75% by 2003. In this web-based database, all PDB entries among individual synchrotron beamlines are archived, synchronized with the weekly PDB release. Statistics regarding the quality of experimental data and the refined model for all structures are presented, and these are analysed to reflect the impact of synchrotron sources. The results confirm the common impression that synchrotron sources extend the size of structures that can be solved with equivalent or better quality than home sources.

CCD-based detector for protein crystallography with synchrotron X-rays☆

A detector with a 114 mm aperture, based on a charge-coupled device (CCD), has been designed for X-ray diffraction studies in protein crystallography. The detector was tested at the National Synchrotron Light Source with a beam intensity, through a 0.3 mm collimator, of greater than 10(9) X-ray photons/s. A fiberoptic taper, an image intensifier, and a lens demagnify, intensify, and focus the image onto a CCD having 512 x 512 pixels. The statistical uncertainty in the detector output was evaluated as a function of conversion gain. From this, a detective quantum efficiency (DQE) of 0.36 was derived. The dynamic range of a 4 x 4 pixel resolution element, comparable in size to a diffraction peak, was 10(4). The point-spread function shows FWHM resolution of approximately 1 pixel, where a pixel is 160-mu-m on the detector face. A data set collected from a chicken egg-white lysozyme crystal, consisting of 495 0.1-degrees frames, was processed by the MADNES data reduction program. The symmetry R-factors for the data were 3.2-3.5%. In a separate experiment a complete lysozyme data set consisting of 45 1-degrees frames was obtained in just 36 s of X-ray exposure. Diffraction images from crystals of the myosin S1 head (a = 275 angstrom) were also recorded; the Bragg spots, only 5 pixels apart, were separated but not fully resolved. Changes in the detector design that will improve the DQE and spatial resolution are outlined. The overall performance showed that this type of detector is well suited for X-ray scattering investigations with synchrotron sources.

Crystallographic structure at 1.6-A resolution of the human adenovirus proteinase in a covalent complex with its 11-amino-acid peptide cofactor: insights on a new fold

The crystal structure of the human adenovirus proteinase (AVP), a cysteine proteinase covalently bound to its 11-amino-acid peptide cofactor pVIc, has been solved to 1.6-A resolution with a crystallographic R-factor of 0.136, R(free)=0.179. The fold of AVP-pVIc is new and the structural basis for it is described in detail. The polypeptide chain of AVP folds into two domains. One domain contains a five-strand beta-sheet with two peripheral alpha-helices; this region represents the hydrophobic core of the protein. A second domain contains the N terminus, several C-terminal alpha-helices, and a small peripheral anti-parallel beta-sheet. The domains interact through an extended polar interface. pVIc spans the two domains like a strap, its C-terminal portion forming a sixth strand on the beta-sheet. The active site is in a long, deep groove located between the two domains. Portions are structurally similar to the active site of the prototypical cysteine proteinase papain, especially some of the Calpha backbone atoms (r.m.s. deviation of 0.354 A for 12 Calpha atoms). The active-site nucleophile of AVP, the conserved Cys(122), was shown to have a pK(a) of 4.5, close to the pK(a) of 3.0 for the nucleophile of papain, suggesting that a similar ion pair arrangement with His(54) may be present in AVP-pVIc. The interactions between AVP and pVIc include 24 non-beta-strand hydrogen bonds, six beta-strand hydrogen bonds and one covalent bond. Of the 204 amino acid residues in AVP, 33 are conserved among the many serotypes of adenovirus, and these aid in forming the active site groove, are involved in substrate specificity or interact between secondary structure elements.

Temporal and spatial control of the adenovirus proteinase by both a peptide and the viral DNA

The adenovirus proteinase (AVP) uses both an 11-amino acid peptide (pVIc) and the viral DNA as cofactors to increase its catalytic rate constant 6000-fold. The crystal structure of an AVP-pVIc complex at 2.6-A resolution reveals a new protein fold of an enzyme that is the first member of a new class of cysteine proteinases, which arose via convergent evolution.